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## Bifurcation Diagrams |
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Well, most likely you already heard something about fractals called 'Bifurcation diagrams' or 'Verhulst diagrams'. If not, well, now you've heard something... Perhaps you've even seen such a fractal. It does not look very aesthetic, so most people do not experiment with it. It makes much more fun creating beautiful images not caring about mathematical sense. If you agree to those people then there is no need to read on. But if you don't agree with them, read on and try to understand the sense behind these diagrams.
Lets examine the model of Verhulst, an example of a bifurcation diagram. It describes how a population of animals (e.g. insects, hares, or something like that) grows from one generation to the next. This model is one of the most simple ones, and additionally it is very interesting and important (for science) so that very much has been written about it in almost every kind of magazines. The model looks just like follows:
(1) x
with 0<=x
The biological meaning of x Now how can we work with this model? Lets start with an example: Lets set x=0.1, a=1.5, n=0, then lets apply the model to these values iteratively:
In this example x
If we repeat this example with a=2.5, then again x In the model of Verhulst there exists an attractor for every value of 'a' between 0 and 4 and one can ask how the attractor depends on 'a', if one increases 'a' in small steps. It seems as if the attractor stays the same for some time, but then suddenly changes. This phenomenon is known as 'bifurcation' (and that's how these fractals got their name). One can create images showing these bifurcations, so called bifurcation diagrams. Lets examine the Verhulst model for different intervals:
In this case x converges to 0, and this is clear, because 'a' is our growth rate, less than 1 ==> dying
Here now the population quickly reaches a balance situation, the population is growing or shrinking (depending on the initial value of x) in a monotone way towards the attractor.
Here still balance occurs, but the successive values of 'x' converge in an oscillating way to the balance-point and not in a monotone way. Now let 'a' be grater than 3 e.g. a=3.1 x1=0.3 If you continue calculating values, then you'll recognize, that 'x' oscillates between two values, 0.557 and 0.764. So here we don't have a balance, the population is oscillating between these two values. If you then take a bigger 'a', but less than 3.449489, then always the population oscillates between 2 values. Starting with a=3.449489 something happens: A so called 'period-doubling' occurs, that means, 'x' suddenly oscillates between 4 values instead of 2. At a=3.5441 this 4-cyclus changes to an 8-cyclus. All these values, at which the cyclus lenght doubles, are called 'bifurcation nodes'. This 8-cyclus mutates to a 16-cyclus, then to a 32-cyclus, etc., upto a specific value: a=3.569946 Now it happens: The whole attractor gets chaotic, that means 'x' oscillates randomly between an infinite amount of unconnected values, here now the attractor is not a cyclus with a fixed length any more, but rather a one dimensional fractal. In this range from 3.569946 upto 4 there are a few 'windows', e.g. at a=3.83, where a 3-cyclus dominates, which mutates to a 6-cyclus, then to a 12-cyclus, a 24-cyclus, etc. 'Windows' like that are spread over the range upto 4.
That's all for now, strange things can happen with such easy models. Last update on Nov 26 2002. |